It is worth noting that the characteristics of the correlation function displayed here at high strain do not exactly resemble the behavior of a liquid. For a liquid above melting temperature, the \(F_s(q,t)\)  shows an exponential decay after the ballistic regime and the \(\beta \) -relaxation part is completely absent [1]}. In case of maximum deformation (\(\dot{\gamma } t = 100\%\) ) used in our simulation, the \(F_s(q,t)\)  shows a signature of two-step relaxation where the \(\beta \) -relaxation is short-lived but present. Also, the \(\tau _r\)  is much higher than the normal liquid. Therefore, the shear molten state in the steady flow regime resembles the nature of viscous supercooled liquids. But unlike the thermally quenched supercooled liquids, these states can not be characterized by its thermodynamic control variables because of the memory effect of the quiescent sample that fades away with strain but is never demolished by any amount of deformation [2]}, [3]} as demonstrated in the next section.
